Article Reference

Total Page:16

File Type:pdf, Size:1020Kb

Article Reference Article Loop corrections and graceful exit in string cosmology FOFFA, Stefano, MAGGIORE, Michele, STURANI, Riccardo Abstract We examine the effect of perturbative string loops on the cosmological pre-big-bang evolution. We study loop corrections derived from heterotic string theory compactified on a $Z_N$ orbifold and we consider the effect of the all-order loop corrections to the Kahler potential and of the corrections to gravitational couplings, including both threshold corrections and corrections due to the mixed Kahler-gravitational anomaly. We find that string loops can drive the evolution into the region of the parameter space where a graceful exit is in principle possible, and we find solutions that, in the string frame, connect smoothly the superinflationary pre-big-bang evolution to a phase where the curvature and the derivative of the dilaton are decreasing. We also find that at a critical coupling the loop corrections to the Kahler potential induce a ghost-like instability, i.e. the kinetic term of the dilaton vanishes. This is similar to what happens in Seiberg-Witten theory and signals the transition to a new regime where the light modes in the effective action are different and are related to the original ones by S-duality. In a [...] Reference FOFFA, Stefano, MAGGIORE, Michele, STURANI, Riccardo. Loop corrections and graceful exit in string cosmology. Nuclear Physics. B, 1999, vol. 552, p. 395-419 DOI : 10.1016/S0550-3213(99)00248-5 Available at: http://archive-ouverte.unige.ch/unige:2212 Disclaimer: layout of this document may differ from the published version. 1 / 1 IFUP-TH 8/99 February 1999 Loop corrections and graceful exit in string cosmology Stefano Foffaa, Michele Maggiorea and Riccardo Sturanib,a (a) Dipartimento di Fisica, via Buonarroti 2, I-56100 Pisa, Italy, and INFN, sezione di Pisa. (b) Scuola Normale Superiore, piazza dei Cavalieri 7, I-56125 Pisa. Abstract We examine the effect of perturbative string loops on the cosmological pre-big-bang evolution. We study loop corrections derived from heterotic string theory compacti- fied on a ZN orbifold and we consider the effect of the all-order loop corrections to the K¨ahler potential and of the corrections to gravitational couplings, including both threshold corrections and corrections due to the mixed K¨ahler-gravitational anomaly. We find that string loops can drive the evolution into the region of the parameter space arXiv:hep-th/9903008v1 28 Feb 1999 where a graceful exit is in principle possible, and we find solutions that, in the string frame, connect smoothly the superinflationary pre-big-bang evolution to a phase where the curvature and the derivative of the dilaton are decreasing. We also find that at a critical coupling the loop corrections to the K¨ahler potential induce a ghost-like insta- bility, i.e. the kinetic term of the dilaton vanishes. This is similar to what happens in Seiberg-Witten theory and signals the transition to a new regime where the light modes in the effective action are different and are related to the original ones by S-duality. In a string context, this means that we enter a D-brane dominated phase. 1 Introduction Pre-big-bang cosmology has been initially developed using the lowest-order effective action of the bosonic string [1]. This allowed to understand the basic features of this cosmological model: the Universe starts at weak coupling and low curvature, follows a superinflationary evolution, and enters a large curvature phase. As long as we are in the perturbative regime, a description with the lowest order effective action is adequate, and can be used to discuss the cosmological evolution [1], the generality of the initial conditions [2], and even to develop some interesting phenomenological consequences concerning the generation of primordial gravitational, axionic, dilatonic and electromagnetic backgrounds [3]. In particular, the low frequency part of these spectra is only sensitive to the low curvature part of the evolution. At lowest order, the cosmological evolution unavoidably reaches large curvatures and strong coupling and finally runs into a singularity. At this stage it is necessary to go beyond the lowest order effective action for understanding how string theory cures the big-bang singularity, and for understanding the matching of pre-big-bang cosmology with standard Friedmann-Robertson-Walker (FRW) post-big-bang cosmology (the so- called ‘graceful exit’ problem [4-12]). One can imagine two possible scenarios. The first is that pertubative corrections succeed in turning the regime of pre-big-bang accelerated expansion into a decelerated expansion, and at the same time the dilaton is attracted by the minimum of its non-perturbative potential. This should take place before entering into a full strong coupling regime, so that perturbative results can still be trusted. In the second scenario the evolution proceeds toward the full strongly coupled regime. In this case one must take into account that at strong coupling and large curvature new light states appear and then the approach based on the effective supergravity action plus string corrections breaks down. The light modes are now different and one must 1 turn to a new effective action, written in terms of the new relevant degrees of freedom. In particular, at strong coupling D-branes [13] are expected to play an important role, since their mass scales like the inverse of the string coupling, 1/g and they are ∼ copiously produced by gravitational fields [14] (see also refs. [15, 16, 17, 18] for related approaches to singularities in string theory). In this paper we investigate how far one can go within the first scenario, analyzing a variety of perturbative string loop corrections. The motivation comes in part from the works [10, 11], where the authors discuss general properties that the loop corrections should have in order to trigger a successful graceful exit. In particular, they find that the corrections should have the appropriate sign, so to induce violation of the null energy condition (NEC), but there should also be a mechanism that at some stage turns them off, otherwise the continued violation of the NEC produces an unbounded growth in the curvature and dilaton. In ref. [11] they presented a model with loop corrections chosen ad hoc, both in the sign and in their functional form, just for the purpose of verifying explicitly on a toy model the general results of ref. [10], and they found that with appropriate choices a complete exit transition is indeed obtained. A transition to a regime of decreasing curvature was also obtained, with a potential chosen ad hoc, in the second paper of ref. [1]. This shows that string loops can in principle trigger a complete graceful exit, but leaves open the question of whether this actually happens for the corrections derived from at least some specific compactification of string theory. In particular, the results of refs. [10, 11] show first of all that the corrections should have the appropriate sign, and this already is an interesting point to check against real string derived corrections, and furthermore they should also have a rather non-trivial functional form that suppresses them at strong coupling. String loop corrections have been much studied in the literature, especially for ZN 2 orbifold compactifications of the heterotic string [19-34], and we can therefore ask whether, at least in some compactification scheme, they fulfill the non-trivial properties needed for a graceful exit. In particular, corrections to the K¨ahler potential are known at all loops; this will be very important for our analysis, since in order to follow the cosmological evolution into the strong coupling regime, a knowledge of the first few terms of the perturbative expansion is not really sufficient, and one must have at least some glimpse into the structure at all loops. After discussing how far one can go within a perturbative approach, we will be able to shed some light on the question of whether perturbative string theory is an adequate tool for discussing string cosmology close to the big-bang singularity, or whether instead non-perturbative string physics plays a crucial role, as in the scenario discussed in ref. [14]. The paper is organized as follows. In sect. 2 we discuss the effective action of the ′ heterotic string with α and loop corrections for a ZN orbifold compactification. In sect. 3 we use these corrections to study the cosmological evolution; we will introduce various corrections one at the time, to understand better their role, and we will find solutions that, in the string frame, smoothly interpolate between the pre-big-bang phase and a phase of decelerated expansion. In sect. 4 we examine the limit of validity of the perturbative approach. We point out that loop corrections induce an instability in the kinetic term of the dilaton, that vanishes at a critical coupling. Similarly to what happens in the Seiberg-Witten model, beyond this value of the coupling the effective action is more appropriately written in terms of variables related to the original ones by S-duality. In string theory this means that there is the onset of a new regime where the light modes of the effective action are given by D-branes rather than by the massless modes of fundamental strings. Sect. 5 contains the conclusions. 3 2 The effective action with loop corrections We consider the effective action of heterotic string theory compactified to four dimen- sions on a ZN orbifold, so that one supersymmetry is left in four dimensions, and we restrict to the graviton-dilaton-moduli sector. In a generic orbifold compactification there are the (1, 2) untwisted moduli fields Ui and the diagonal (1, 1) untwisted moduli fields Ti (non-diagonal moduli are included in the matter fields).
Recommended publications
  • A Space-Time Orbifold: a Toy Model for a Cosmological Singularity
    hep-th/0202187 UPR-981-T, HIP-2002-07/TH A Space-Time Orbifold: A Toy Model for a Cosmological Singularity Vijay Balasubramanian,1 ∗ S. F. Hassan,2† Esko Keski-Vakkuri,2‡ and Asad Naqvi1§ 1David Rittenhouse Laboratories, University of Pennsylvania Philadelphia, PA 19104, U.S.A. 2Helsinki Institute of Physics, P.O.Box 64, FIN-00014 University of Helsinki, Finland Abstract We explore bosonic strings and Type II superstrings in the simplest time dependent backgrounds, namely orbifolds of Minkowski space by time reversal and some spatial reflections. We show that there are no negative norm physi- cal excitations. However, the contributions of negative norm virtual states to quantum loops do not cancel, showing that a ghost-free gauge cannot be chosen. The spectrum includes a twisted sector, with strings confined to a “conical” sin- gularity which is localized in time. Since these localized strings are not visible to asymptotic observers, interesting issues arise regarding unitarity of the S- matrix for scattering of propagating states. The partition function of our model is modular invariant, and for the superstring, the zero momentum dilaton tad- pole vanishes. Many of the issues we study will be generic to time-dependent arXiv:hep-th/0202187v2 19 Apr 2002 cosmological backgrounds with singularities localized in time, and we derive some general lessons about quantizing strings on such spaces. 1 Introduction Time-dependent space-times are difficult to study, both classically and quantum me- chanically. For example, non-static solutions are harder to find in General Relativity, while the notion of a particle is difficult to define clearly in field theory on time- dependent backgrounds.
    [Show full text]
  • Deformations of G2-Structures, String Dualities and Flat Higgs Bundles Rodrigo De Menezes Barbosa University of Pennsylvania, [email protected]
    University of Pennsylvania ScholarlyCommons Publicly Accessible Penn Dissertations 2019 Deformations Of G2-Structures, String Dualities And Flat Higgs Bundles Rodrigo De Menezes Barbosa University of Pennsylvania, [email protected] Follow this and additional works at: https://repository.upenn.edu/edissertations Part of the Mathematics Commons, and the Quantum Physics Commons Recommended Citation Barbosa, Rodrigo De Menezes, "Deformations Of G2-Structures, String Dualities And Flat Higgs Bundles" (2019). Publicly Accessible Penn Dissertations. 3279. https://repository.upenn.edu/edissertations/3279 This paper is posted at ScholarlyCommons. https://repository.upenn.edu/edissertations/3279 For more information, please contact [email protected]. Deformations Of G2-Structures, String Dualities And Flat Higgs Bundles Abstract We study M-theory compactifications on G2-orbifolds and their resolutions given by total spaces of coassociative ALE-fibrations over a compact flat Riemannian 3-manifold Q. The afl tness condition allows an explicit description of the deformation space of closed G2-structures, and hence also the moduli space of supersymmetric vacua: it is modeled by flat sections of a bundle of Brieskorn-Grothendieck resolutions over Q. Moreover, when instanton corrections are neglected, we obtain an explicit description of the moduli space for the dual type IIA string compactification. The two moduli spaces are shown to be isomorphic for an important example involving A1-singularities, and the result is conjectured to hold in generality. We also discuss an interpretation of the IIA moduli space in terms of "flat Higgs bundles" on Q and explain how it suggests a new approach to SYZ mirror symmetry, while also providing a description of G2-structures in terms of B-branes.
    [Show full text]
  • Jhep05(2019)105
    Published for SISSA by Springer Received: March 21, 2019 Accepted: May 7, 2019 Published: May 20, 2019 Modular symmetries and the swampland conjectures JHEP05(2019)105 E. Gonzalo,a;b L.E. Ib´a~neza;b and A.M. Urangaa aInstituto de F´ısica Te´orica IFT-UAM/CSIC, C/ Nicol´as Cabrera 13-15, Campus de Cantoblanco, 28049 Madrid, Spain bDepartamento de F´ısica Te´orica, Facultad de Ciencias, Universidad Aut´onomade Madrid, 28049 Madrid, Spain E-mail: [email protected], [email protected], [email protected] Abstract: Recent string theory tests of swampland ideas like the distance or the dS conjectures have been performed at weak coupling. Testing these ideas beyond the weak coupling regime remains challenging. We propose to exploit the modular symmetries of the moduli effective action to check swampland constraints beyond perturbation theory. As an example we study the case of heterotic 4d N = 1 compactifications, whose non-perturbative effective action is known to be invariant under modular symmetries acting on the K¨ahler and complex structure moduli, in particular SL(2; Z) T-dualities (or subgroups thereof) for 4d heterotic or orbifold compactifications. Remarkably, in models with non-perturbative superpotentials, the corresponding duality invariant potentials diverge at points at infinite distance in moduli space. The divergence relates to towers of states becoming light, in agreement with the distance conjecture. We discuss specific examples of this behavior based on gaugino condensation in heterotic orbifolds. We show that these examples are dual to compactifications of type I' or Horava-Witten theory, in which the SL(2; Z) acts on the complex structure of an underlying 2-torus, and the tower of light states correspond to D0-branes or M-theory KK modes.
    [Show full text]
  • Arxiv:Hep-Th/9404101V3 21 Nov 1995
    hep-th/9404101 April 1994 Chern-Simons Gauge Theory on Orbifolds: Open Strings from Three Dimensions ⋆ Petr Horavaˇ ∗ Enrico Fermi Institute University of Chicago 5640 South Ellis Avenue Chicago IL 60637, USA ABSTRACT Chern-Simons gauge theory is formulated on three dimensional Z2 orbifolds. The locus of singular points on a given orbifold is equivalent to a link of Wilson lines. This allows one to reduce any correlation function on orbifolds to a sum of more complicated correlation functions in the simpler theory on manifolds. Chern-Simons theory on manifolds is known arXiv:hep-th/9404101v3 21 Nov 1995 to be related to 2D CFT on closed string surfaces; here I show that the theory on orbifolds is related to 2D CFT of unoriented closed and open string models, i.e. to worldsheet orb- ifold models. In particular, the boundary components of the worldsheet correspond to the components of the singular locus in the 3D orbifold. This correspondence leads to a simple identification of the open string spectra, including their Chan-Paton degeneration, in terms of fusing Wilson lines in the corresponding Chern-Simons theory. The correspondence is studied in detail, and some exactly solvable examples are presented. Some of these examples indicate that it is natural to think of the orbifold group Z2 as a part of the gauge group of the Chern-Simons theory, thus generalizing the standard definition of gauge theories. E-mail address: [email protected] ⋆∗ Address after September 1, 1994: Joseph Henry Laboratories, Princeton University, Princeton, New Jersey 08544. 1. Introduction Since the first appearance of the notion of “orbifolds” in Thurston’s 1977 lectures on three dimensional topology [1], orbifolds have become very appealing objects for physicists.
    [Show full text]
  • An Introduction to Orbifolds
    An introduction to orbifolds Joan Porti UAB Subdivide and Tile: Triangulating spaces for understanding the world Lorentz Center November 2009 An introduction to orbifolds – p.1/20 Motivation • Γ < Isom(Rn) or Hn discrete and acts properly discontinuously (e.g. a group of symmetries of a tessellation). • If Γ has no fixed points ⇒ Γ\Rn is a manifold. • If Γ has fixed points ⇒ Γ\Rn is an orbifold. An introduction to orbifolds – p.2/20 Motivation • Γ < Isom(Rn) or Hn discrete and acts properly discontinuously (e.g. a group of symmetries of a tessellation). • If Γ has no fixed points ⇒ Γ\Rn is a manifold. • If Γ has fixed points ⇒ Γ\Rn is an orbifold. ··· (there are other notions of orbifold in algebraic geometry, string theory or using grupoids) An introduction to orbifolds – p.2/20 Examples: tessellations of Euclidean plane Γ= h(x, y) → (x + 1, y), (x, y) → (x, y + 1)i =∼ Z2 Γ\R2 =∼ T 2 = S1 × S1 An introduction to orbifolds – p.3/20 Examples: tessellations of Euclidean plane Rotations of angle π around red points (order 2) An introduction to orbifolds – p.3/20 Examples: tessellations of Euclidean plane Rotations of angle π around red points (order 2) 2 2 An introduction to orbifolds – p.3/20 Examples: tessellations of Euclidean plane Rotations of angle π around red points (order 2) 2 2 2 2 2 2 2 2 2 2 2 2 An introduction to orbifolds – p.3/20 Example: tessellations of hyperbolic plane Rotations of angle π, π/2 and π/3 around vertices (order 2, 4, and 6) An introduction to orbifolds – p.4/20 Example: tessellations of hyperbolic plane Rotations of angle π, π/2 and π/3 around vertices (order 2, 4, and 6) 2 4 2 6 An introduction to orbifolds – p.4/20 Definition Informal Definition • An orbifold O is a metrizable topological space equipped with an atlas modelled on Rn/Γ, Γ < O(n) finite, with some compatibility condition.
    [Show full text]
  • Ads Orbifolds and Penrose Limits
    IPM/P-2002/061 UCB-PTH-02/54 LBL-51767 hep-th/yymmnnn AdS orbifolds and Penrose limits Mohsen Alishahihaa, Mohammad M. Sheikh-Jabbarib and Radu Tatarc a Institute for Studies in Theoretical Physics and Mathematics (IPM) P.O.Box 19395-5531, Tehran, Iran e-mail: [email protected] b Department of Physics, Stanford University 382 via Pueblo Mall, Stanford CA 94305-4060, USA e-mail: [email protected] c Department of Physics, 366 Le Conte Hall University of California, Berkeley, CA 94720 and Lawrence Berkeley National Laboratory Berkeley, CA 94720 email:[email protected] Abstract In this paper we study the Penrose limit of AdS5 orbifolds. The orbifold can be either in the pure spatial directions or space and time directions. For the AdS =¡ S5 spatial orbifold we observe that after the Penrose limit we 5 £ obtain the same result as the Penrose limit of AdS S5=¡. We identify the 5 £ corresponding BMN operators in terms of operators of the gauge theory on R £ S3=¡. The semi-classical description of rotating strings in these backgrounds have also been studied. For the spatial AdS orbifold we show that in the quadratic order the obtained action for the fluctuations is the same as that in S5 orbifold, however, the higher loop correction can distinguish between two cases. 1 Introduction In the past ¯ve years important results have been obtained relating closed and open string theories, in particular the AdS/CFT correspondence [1] had important impact into the understanding between these two sectors. The main problem in testing the conjecture beyond the supergravity level is the fact that we do not know how to quantize string theory in the presence of RR-fluxes.
    [Show full text]
  • K3 Surfaces and String Duality
    RU-96-98 hep-th/9611137 November 1996 K3 Surfaces and String Duality Paul S. Aspinwall Dept. of Physics and Astronomy, Rutgers University, Piscataway, NJ 08855 ABSTRACT The primary purpose of these lecture notes is to explore the moduli space of type IIA, type IIB, and heterotic string compactified on a K3 surface. The main tool which is invoked is that of string duality. K3 surfaces provide a fascinating arena for string compactification as they are not trivial spaces but are sufficiently simple for one to be able to analyze most of their properties in detail. They also make an almost ubiquitous appearance in the common statements concerning string duality. We arXiv:hep-th/9611137v5 7 Sep 1999 review the necessary facts concerning the classical geometry of K3 surfaces that will be needed and then we review “old string theory” on K3 surfaces in terms of conformal field theory. The type IIA string, the type IIB string, the E E heterotic string, 8 × 8 and Spin(32)/Z2 heterotic string on a K3 surface are then each analyzed in turn. The discussion is biased in favour of purely geometric notions concerning the K3 surface itself. Contents 1 Introduction 2 2 Classical Geometry 4 2.1 Definition ..................................... 4 2.2 Holonomy ..................................... 7 2.3 Moduli space of complex structures . ..... 9 2.4 Einsteinmetrics................................. 12 2.5 AlgebraicK3Surfaces ............................. 15 2.6 Orbifoldsandblow-ups. .. 17 3 The World-Sheet Perspective 25 3.1 TheNonlinearSigmaModel . 25 3.2 TheTeichm¨ullerspace . .. 27 3.3 Thegeometricsymmetries . .. 29 3.4 Mirrorsymmetry ................................. 31 3.5 Conformalfieldtheoryonatorus . ... 33 4 Type II String Theory 37 4.1 Target space supergravity and compactification .
    [Show full text]
  • International Theoretical Physics
    INTERNATIONAL THEORETICAL PHYSICS INTERACTION OF MOVING D-BRANES ON ORBIFOLDS INTERNATIONAL ATOMIC ENERGY Faheem Hussain AGENCY Roberto Iengo Carmen Nunez UNITED NATIONS and EDUCATIONAL, Claudio A. Scrucca SCIENTIFIC AND CULTURAL ORGANIZATION CD MIRAMARE-TRIESTE 2| 2i CO i IC/97/56 ABSTRACT SISSAREF-/97/EP/80 We use the boundary state formalism to study the interaction of two moving identical United Nations Educational Scientific and Cultural Organization D-branes in the Type II superstring theory compactified on orbifolds. By computing the and velocity dependence of the amplitude in the limit of large separation we can identify the International Atomic Energy Agency nature of the different forces between the branes. In particular, in the Z orbifokl case we THE ABDUS SALAM INTERNATIONAL CENTRE FOR THEORETICAL PHYSICS 3 find a boundary state which is coupled only to the N = 2 graviton multiplet containing just a graviton and a vector like in the extremal Reissner-Nordstrom configuration. We also discuss other cases including T4/Z2. INTERACTION OF MOVING D-BRANES ON ORBIFOLDS Faheem Hussain The Abdus Salam International Centre for Theoretical Physics, Trieste, Italy, Roberto Iengo International School for Advanced Studies, Trieste, Italy and INFN, Sezione di Trieste, Trieste, Italy, Carmen Nunez1 Instituto de Astronomi'a y Fisica del Espacio (CONICET), Buenos Aires, Argentina and Claudio A. Scrucca International School for Advanced Studies, Trieste, Italy and INFN, Sezione di Trieste, Trieste, Italy. MIRAMARE - TRIESTE February 1998 1 Regular Associate of the ICTP. The non-relativistic dynamics of Dirichlet branes [1-3], plays an essential role in the coordinate satisfies Neumann boundary conditions, dTX°(T = 0, a) = drX°(r = I, a) = 0.
    [Show full text]
  • Orbifolds Orbifolds As Quotients of Manifolds by Lie Group Actions Stratification of Orbifolds
    Definition and Examples of Orbifolds Orbifolds as quotients of manifolds by Lie group actions Stratification of orbifolds ORBIFOLDS July 16, 2010 ORBIFOLDS Definition and Examples of Orbifolds Orbifolds as quotients of manifolds by Lie group actions Stratification of orbifolds Outline 1 Definition and Examples of Orbifolds 2 Orbifolds as quotients of manifolds by Lie group actions 3 Stratification of orbifolds ORBIFOLDS Definition and Examples of Orbifolds Orbifolds as quotients of manifolds by Lie group actions Stratification of orbifolds Outline 1 Definition and Examples of Orbifolds 2 Orbifolds as quotients of manifolds by Lie group actions 3 Stratification of orbifolds ORBIFOLDS Definition and Examples of Orbifolds Orbifolds as quotients of manifolds by Lie group actions Stratification of orbifolds What is an orbifold? Definition An n-dimensional orbifold O is a second countable Hausdorff topological space together with a maximal n-dimensional orbifold atlas. Definition An orbifold atlas is a collection of mutually compatible orbifold charts whose images cover O. So what’s an orbifold chart? ORBIFOLDS Definition and Examples of Orbifolds Orbifolds as quotients of manifolds by Lie group actions Stratification of orbifolds What is an orbifold? Definition An n-dimensional orbifold O is a second countable Hausdorff topological space together with a maximal n-dimensional orbifold atlas. Definition An orbifold atlas is a collection of mutually compatible orbifold charts whose images cover O. So what’s an orbifold chart? ORBIFOLDS Definition and Examples of Orbifolds Orbifolds as quotients of manifolds by Lie group actions Stratification of orbifolds What is an orbifold? Definition An n-dimensional orbifold O is a second countable Hausdorff topological space together with a maximal n-dimensional orbifold atlas.
    [Show full text]
  • Lectures on D-Branes, Gauge Theories and Calabi-Yau
    UPR-1086-T Lectures on D-branes, Gauge Theories and Calabi-Yau Singularities Yang-Hui He Department of Physics and Math/Physics RG University of Pennsylvania Philadelphia, PA 19104–6396, USA Abstract These lectures, given at the Chinese Academy of Sciences for the BeiJing/HangZhou International Summer School in Mathematical Physics, are intended to introduce, to the beginning student in string theory and mathematical physics, aspects of the rich and beautiful subject of D-brane gauge theories constructed from local Calabi-Yau spaces. arXiv:hep-th/0408142v1 18 Aug 2004 Topics such as orbifolds, toric singularities, del Pezzo surfaces as well as chaotic duality will be covered. ∗[email protected] Contents 1 Introduction 2 2 Minute Waltz on the String 5 2.1 The D3-brane in R1,9 ............................... 6 2.2 D3-branesonCalabi-Yauthreefolds . ...... 7 3 The Simplest Case: S = C3 8 4 Orbifolds and Quivers 10 4.1 ProjectiontoDaughterTheories. ..... 10 4.2 Quivers ...................................... 12 4.3 TheMcKayCorrespondence . 12 4.4 McKay, Dimension 2 and N =2......................... 15 4.5 N = 1 Theories and C3 Orbifolds ........................ 15 4.6 Quivers, Modular Invariants, Path Algebras? . ......... 17 4.7 MoreGames.................................... 17 5 Gauge Theories, Moduli Spaces andSymplectic Quotients 19 5.1 QuiverGaugeTheory............................... 20 5.2 An Illustrative Example: The Conifold . ...... 21 5.3 ToricSingularities.. .. .. ... 22 5.3.1 A Lightning Review on Toric Varieties . ... 23 5.3.2 Witten’s Gauged Linear Sigma Model (GLSM) . .. 23 5.4 TheForwardAlgorithm ............................. 24 5.4.1 Forward Algorithm for Abelian Orbifolds . ..... 25 5.5 TheInverseAlgorithm ............................. 28 5.6 Applications of Inverse Algorithm . ...... 29 5.6.1 delPezzoSurfaces ...........................
    [Show full text]
  • Introduction to Vertex Operator Algebras I 1 Introduction
    数理解析研究所講究録 904 巻 1995 年 1-25 1 Introduction to vertex operator algebras I Chongying Dong1 Department of Mathematics, University of California, Santa Cruz, CA 95064 1 Introduction The theory of vertex (operator) algebras has developed rapidly in the last few years. These rich algebraic structures provide the proper formulation for the moonshine module construction for the Monster group ([BI-B2], [FLMI], [FLM3]) and also give a lot of new insight into the representation theory of the Virasoro algebra and affine Kac-Moody algebras (see for instance [DL3], [DMZ], [FZ], [W]). The modern notion of chiral algebra in conformal field theory [BPZ] in physics essentially corresponds to the mathematical notion of vertex operator algebra; see e.g. [MS]. This is the first part of three consecutive lectures by Huang, Li and myself. In this part we are mainly concerned with the definitions of vertex operator algebras, twisted modules and examples. The second part by Li is about the duality and local systems and the third part by Huang is devoted to the contragradient modules and geometric interpretations of vertex operator algebras. (We refer the reader to Li and Huang’s lecture notes for the related topics.) So many exciting topics are not covered in these three lectures. The book [FHL] is an excellent introduction to the subject. There are also existing papers [H1], [Ge] and [P] which review the axiomatic definition of vertex operator algebras, geometric interpretation of vertex operator algebras, the connection with conformal field theory, Borcherds algebras and the monster Lie algebra. Most work on vertex operator algebras has been concentrated on the concrete exam- ples of vertex operator algebras and the representation theory.
    [Show full text]
  • D-Branes on Orbifolds with Discrete Torsion and Topological Obstruction
    Received: March 27, 2000, Accepted: May 3, 2000 HYPER VERSION D-branes on orbifolds with discrete torsion and topological obstruction Jaume Gomis JHEP05(2000)006 Department of Physics, California Institute of Technology Pasadena, CA 91125, USA, and Caltech-USC Center for Theoretical Physics, University of Southern California Los Angeles, CA 90089 E-mail: [email protected] Abstract: We find the orbifold analog of the topological relation recently found by Freed and Witten which restricts the allowed D-brane configurations of type-II vacua with a topologically non-trivial flat B-field. The result relies in Douglas proposal — which we derive from worldsheet consistency conditions — of embedding projective representations on open string Chan-Paton factors when considering orbifolds with discrete torsion. The orbifold action on open strings gives a natural definition of the algebraic K-theory group — using twisted cross products — responsible for measur- ing Ramond-Ramond charges in orbifolds with discrete torsion. We show that the correspondence between fractional branes and Ramond-Ramond fields follows in an interesting fashion from the way that discrete torsion is implemented on open and closed strings. Keywords: D-branes, Superstring Vacua, Conformal Field Models in String Theory. Contents 1. Introduction, results and conclusions 1 2. Open and closed strings in orbifolds with discrete torsion 5 3. Examples and D-brane charges 9 JHEP05(2000)006 1. Introduction, results and conclusions Orbifolds [1] in string theory provide a tractable arena where CFT can be used to describe perturbative vacua. In the more conventional geometric compactifications, geometry and topology provide powerful techniques in describing the long wavelength approximation to string theory.
    [Show full text]